Astraeus V: the emergence and evolution of metallicity scaling relations during the epoch of reionization

Author:

Ucci Graziano1ORCID,Dayal Pratika1ORCID,Hutter Anne1ORCID,Kobayashi Chiaki2ORCID,Gottlöber Stefan3,Yepes Gustavo45ORCID,Hunt Leslie6ORCID,Legrand Laurent1ORCID,Tortora Crescenzo67ORCID

Affiliation:

1. Kapteyn Astronomical Institute, University of Groningen , P.O. Box 800, NL-9700 AV Groningen, the Netherlands

2. Centre for Astrophysics Research, Department of Physics, Astronomy and Mathematics, University of Hertfordshire , College Lane, Hatfield, Hertfordshire AL10 9AB, UK

3. Leibniz-Institut für Astrophysik , An der Sternwarte 16, D-14482 Potsdam, Germany

4. Departamento de Fisica Teorica, Modulo 8, Facultad de Ciencias, Universidad Autonoma de Madrid , E-28049 Madrid, Spain

5. CIAFF, Facultad de Ciencias, Universidad Autonoma de Madrid , E-28049 Madrid, Spain

6. INAF -Osservatorio Astrofisico di Arcetri , Largo E. Fermi 5, I-50125 Firenze, Italy

7. INAF -Osservatorio Astronomico di Capodimonte , Salita Moiariello 16, I-80131 Napoli, Italy

Abstract

ABSTRACT In this work, we have implemented a detailed physical model of galaxy chemical enrichment into the Astraeus (seminumerical rAdiative tranSfer coupling of galaxy formaTion and Reionization in N-body dark matter simUlationS) framework which couples galaxy formation and reionization in the first billion years. Simulating galaxies spanning over 2.5 orders of magnitude in halo mass with $M_{\rm h} \sim 10^{8.9}{-}10^{11.5}\,{\rm M_\odot}$ ($M_{\rm h} \sim 10^{8.9}{-}10^{12.8}\rm M_\odot$) at z ∼ 10 (5), we find: (i) smooth accretion of metal-poor gas from the intergalactic medium (IGM) plays a key role in diluting the interstellar medium interstellar medium metallicity which is effectively restored due to self-enrichment from star formation; (ii) a redshift averaged gas-mass loading factor that depends on the stellar mass as $\eta _{\rm g} \approx 1.38 ({M_*}/{10^{10}\, {\rm \rm M_\odot }})^{-0.43}$; (iii) the mass–metallicity relation is already in place at z ∼ 10 and shows effectively no redshift evolution down to z ∼ 5; (iv) for a given stellar mass, the metallicity decreases with an increase in the star formation rate (SFR); (v) the key properties of the gas-phase metallicity (in units of 12 + log(O/H), stellar mass, SFR and redshift are linked through a high-redshift fundamental plane of metallicity (HFPZ) for which we provide a functional form; (vi) the mass–metallicity–SFR relations are effectively independent of the reionization radiative feedback model for $M_* {\,\, \buildrel\gt \over \sim \,\,}10^{6.5}\rm M_\odot$ galaxies; (vii) while low-mass galaxies ($M_{\rm h} {\,\, \buildrel\lt \over \sim \,\,}10^9\,\rm M_\odot$) are the key contributors to the metal budget of the IGM at early times, higher mass haloes provide about 50 per cent of the metal budget at lower redshifts.

Funder

European Research Council

NWO

University of Groningen

Science and Technology Facilities Council

FEDER

GCS

Leibniz Institute for Astrophysics Potsdam

Publisher

Oxford University Press (OUP)

Subject

Space and Planetary Science,Astronomy and Astrophysics

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